Magnetoresistive sensor having low resistivity dual path conductor and optimized magnetic
Summary by NHIP
Low resistivity dual path conductor magnetoresistive sensor
The transducing head features a magnetoresistive sensor positioned between two abutted dual path conductor/magnet structures. Each structure contains a bias layer with 1 to 5 kOe coercivity and greater than 0.8 squareness, formed on a seed layer atop chromium, ruthenium, tantalum, titanium, or tungsten conductor layers.
Claim Score by NHIP
Abstract
A transducing head has a magnetoresistive sensor and a first and a second dual path conductor/magnet structure for providing current to the magnetoresistive sensor and for stabilizing the magnetoresistive sensor. The first and the second dual path conductor/magnet structures are arranged in an abutted-junction configuration on opposite sides of the magnetoresistive sensor. Each of the first and the second dual path conductor/magnet structures has at least one bias layer and at least one conductor layer. Each bias layer is formed upon a bias seed layer positioned over one of the conductor layers. Each bias seed layer is selected to result in the bias layer formed upon it having a coercivity between about 1 kOe and about 5 kOe and an in-plane remnant squareness greater than about 0.8. Most preferably, each of the first and the second dual path conductor/magnet structures is formed of at least two conductor layers interspersed with at least one bias layer.

Term
Term ended
Expired 26 June 2023, 3.2 years ago.
- Priority
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19 claims: 5 independent, 14 dependent
- 1Broadest claimClaim Score 66, broad(NHIP)A transducing head comprising:a first and a second dual path conductor/magnet structure each comprising a bias layer positioned between a first conductor layer and a second conductor layer and a bias seed layer upon which the bias layer is formed, the bias seed layer being selected to result in the bias layer having a coercivity between about 1 kOe and about 5 kOe and an in-plane remnant squareness greater than about 0.8;and a magnetoresistive sensor positioned between the first and the second dual path conductor/magnet structures, the magnetoresistive sensor being formed of a plurality of layers that are each substantially parallel to the layers of the first and the second dual path conductor/magnet structures.
- 11A transducing head comprising:a magnetoresistive sensor;a first conductor layer positioned on a first side of the magnetoresistive sensor;a second conductor layer positioned on a second side of the magnetoresistive sensor;a first bias seed layer positioned over the first conductor layer and formed of a material selected from the group consisting of chromium, ruthenium, tantalum, titanium, tungsten and alloys based primarily on materials selected from the group consisting of chromium, ruthenium, tantalum, titanium, and tungsten;a second bias seed layer positioned over the second conductor layer and formed of a material selected from the group consisting of chromium, ruthenium, tantalum, titanium, tungsten and alloys based primarily on materials selected from the group consisting of chromium, ruthenium, tantalum, titanium, and tungsten;a first bias layer positioned over the first bias seed layer, wherein the first bias layer is formed of a hard magnetic material;and a second bias layer positioned over the second bias seed layer, wherein the second bias layer is formed of a hard magnetic material.
- 17A transducing head comprising:a spin valve sensor comprising a spacer layer positioned between a free layer and a pinned layer;and means for providing a current to the spin valve sensor and for stabilizing the free layer of the spin valve sensor, wherein the means comprises a first and a second structure each comprising a bias layer formed of a hard magnetic material positioned between a first conductor layer and a second conductor layer and a bias seed layer upon which the bias layer is formed, the first and the second structures being arranged in an abutted-junction configuration on opposite sides of the spin valve sensor.
- 18A transducing head comprising:a spin valve sensor comprising a spacer layer positioned between a free layer and a pinned layer;and means for providing a current to the spin valve sensor and for stabilizing the free layer of the spin valve sensor, wherein the means comprises a first and a second laminate structure comprising at least two conductor layers interspersed with at least one bias layer, wherein each bias layer is formed of a hard magnetic material, each bias layer being formed upon a bias seed layer formed of a material selected from the group consisting of tantalum, titanium-tungsten, and chromium, the first and the second laminate structures being arranged in an abutted-junction configuration on opposite sides of the spin valve sensor.
- 19A transducing head comprising:a spin valve sensor comprising a spacer layer positioned between a free layer and a pinned layer;means for providing a current to the spin valve sensor and for stabilizing the free layer of the spin valve sensor, wherein the means comprises: a first and a second conductor layer abutted with opposite sides of the spin valve sensor;a first and a second bias seed layer abutted with opposite sides of the spin valve sensor and positioned above a respective one of the first and the second conductor layers;and a first and a second bias layer abutted with opposite sides of the spin valve sensor and positioned above a respective one of the first and the second bias seed layers, wherein the first and second bias layers are formed of a hard magnetic material.
Independent claims5
48 paragraphs in 5 sections, as filed
CROSS-REFERENCE TO RELATED APPLICATION(S)
This application claims priority from provisional U.S. patent application Ser. No. 60/297,542 of David James Larson and Eric Walter Singleton, filed on Jun. 12, 2001 and entitled “Magnetoresistive Sensor Having Low Resistivity Dual Path Conductor and Optimized Magnetic Layer”.
BACKGROUND OF THE INVENTION
The present invention relates generally to the field of magnetic data storage and retrieval systems. More particularly, the present invention relates to a transducing head having a magnetoresistive sensor and first and second dual path conductor/magnet structures arranged in an abutted-junction configuration on opposite sides of the magnetoresistive sensor for stabilizing and for providing current to the magnetoresistive sensor.
A transducing head of a magnetic data storage and retrieval system typically includes a magnetoresistive (MR) reader portion for retrieving magnetic data stored on a magnetic media. The reader is typically formed of several layers which include an MR sensor positioned between two gap layers, which are in turn positioned between two magnetically permeable shield layers. The MR sensor may be any one of a plurality of MR-type sensors, including, but not limited to, anisotropic magnetoresistive (AMR), giant magnetoresistive (GMR), spin valve and spin tunneling sensors.
When the transducing head is placed near a magnetic medium, a resistance of the MR sensor fluctuates in response to a magnetic field emanating from written transitions in the magnetic medium. By providing a sense current through the MR sensor, the resistance of the sensor can be measured and used by external circuitry to decipher the information stored on the magnetic medium. The sense current is provided to the MR sensor via a pair of current contacts.
To operate the MR sensor properly, the sensor must be stabilized against the formation of edge domains because domain wall motion results in electrical noise that makes data recovery impossible. A common way to achieve stabilization is with a permanent magnet abutted junction configuration in which permanent magnet bias elements directly abut opposite sides of the MR sensor. Permanent magnets have a high coercive field (i.e., are hard magnets). The magnetostatic field from the permanent magnets stabilizes the MR sensor, prevents edge domain formation, and provides proper bias.
In recent years, MR sensor widths have decreased to accommodate ever-increasing areal densities of magnetic media. This decrease in MR sensor widths has resulted in increased MR sensor resistivity, which undesirably requires the new design of the external circuitry used to decipher the information stored on the magnetic medium. Thus, there is a need for a MR sensor design that allows for decreased sensor widths without increasing the MR sensor resistivity.
BRIEF SUMMARY OF THE INVENTION
A transducing head has a magnetoresistive sensor and a first and a second dual path conductor/magnet structure for providing current to the magnetoresistive sensor and for stabilizing the magnetoresistive sensor. The first and the second dual path conductor/magnet structures are arranged in an abutted-junction configuration on opposite sides of the magnetoresistive sensor. Each of the first and the second dual path conductor/magnet structures has at least one bias layer and at least one conductor layer. Each bias layer is formed upon a bias seed layer positioned over one of the conductor layers. Each bias seed layer is selected to result in the bias layer formed upon it having a coercivity between about 1 kOe and about 5 kOe and an in-plane remnant squareness greater than about 0.8. Most preferably, each of the first and the second dual path conductor/magnet structures is formed of at least two conductor layers interspersed with at least one bias layer.
BRIEF DESCRIPTION OF THE DRAWINGS
<figref idref="DRAWINGS">FIG. 1</figref> is cross-sectional view of a transducing head in accord with the present invention.
<figref idref="DRAWINGS">FIG. 2</figref> is a cross-sectional view of a transducing head in accord with an alternate embodiment of the present invention.
<figref idref="DRAWINGS">FIG. 3</figref> is a layer diagram of a spin valve sensor configured as a bottom spin valve.
<figref idref="DRAWINGS">FIG. 4</figref> is a layer diagram of a spin valve sensor configured as a dual spin valve.
<figref idref="DRAWINGS">FIG. 5</figref> is a cross-sectional view of a prior art transducing head.
<figref idref="DRAWINGS">FIG. 6</figref> is a cross-sectional view of the transducing head of <figref idref="DRAWINGS">FIG. 1</figref> taken along cross-section VI—VI.
<figref idref="DRAWINGS">FIG. 7</figref> is a cross-sectional view of the transducing head of <figref idref="DRAWINGS">FIG. 5</figref> taken along cross-section VII—VII.
<figref idref="DRAWINGS">FIGS. 8 and 9</figref> are charts comparing resistivity of the transducing head of <figref idref="DRAWINGS">FIG. 1</figref> to the resistivity of the prior art transducing head of FIG. <b>5</b>.
<figref idref="DRAWINGS">FIG. 10</figref> is a graph comparing current distribution through a spacer layer of a spin valve sensor of a transducing head in accord with the present invention with current distribution through a spacer layer of a spin valve sensor of a prior art transducing head.
DETAILED DESCRIPTION
<figref idref="DRAWINGS">FIG. 1</figref> is a cross-sectional view of transducing head <b>10</b> in accord with the present invention. Transducing head <b>10</b> includes first gap layer <b>12</b>, sensor seed layer <b>14</b>, magnetoresistive (MR) sensor <b>16</b>, cap layer <b>18</b>, first dual path conductor/magnet structure <b>20</b>, second dual path conductor/magnet structure <b>22</b> and second gap layer <b>24</b>.
Sensor seed layer <b>14</b> is formed on a central region of insulating first gap layer <b>12</b>. MR sensor <b>16</b> is formed on sensor seed layer <b>14</b>. MR sensor <b>16</b> is a multilayer device operable to sense magnetic flux from a magnetic media (not illustrated in FIG. <b>1</b>). MR sensor <b>16</b> may be any one of a plurality of MR-type sensors, including, but not limited to, anisotropic magnetoresistive (AMR), giant magnetoresistive (GMR), spin valve, and spin tunneling sensors. At least one layer of MR sensor <b>16</b> is a sensing layer, such as a free layer of a GMR spin valve sensor that requires longitudinal biasing. Cap layer <b>18</b> is positioned on MR sensor <b>16</b>.
First and second dual path conductor/magnet structures <b>20</b> and <b>22</b> are arranged on end portions of first gap layer <b>12</b> in an abutted-junction configuration on opposite sides of MR sensor <b>16</b>. First and second dual path conductor/magnet structures <b>20</b> and <b>22</b> function to provide current to MR sensor <b>16</b> and to provide longitudinal biasing to the sensing layer of MR sensor <b>16</b>. Insulating second gap layer <b>24</b> is positioned over cap layer <b>18</b> and first and second dual path conductor/magnetic structures <b>20</b> and <b>22</b>.
First dual path conductor/magnet structure <b>20</b> is sequentially formed of first contact seed layer <b>26</b>, first contact <b>28</b>, bias seed layer <b>30</b>, bias layer <b>32</b>, and second contact <b>34</b>. Similarly, second dual path conductor/magnet structure <b>22</b> is sequentially formed of first contact seed layer <b>36</b>, first contact <b>38</b>, bias seed layer <b>40</b>, bias layer <b>42</b>, and second contact <b>44</b>.
First contact seed layers <b>26</b> and <b>36</b> are each preferably formed of an about 50 Å to about 200 Å thick layer of a material selected to promote the texture and grain growth of each subsequently formed layer. More preferably, first contact seed layers <b>26</b> and <b>36</b> are formed of a material such as chromium, ruthenium, tantalum, titanium, tungsten or alloy based primarily of chromium, ruthenium, tantalum, titanium, and/or tungsten.
First contacts <b>28</b> and <b>38</b> are each preferably formed of an about 100 Å to about 1000 Å thick layer of a low resistivity material, such as chromium, copper, gold, rhodium, ruthenium, silver, tantalum, tungsten, or an alloy based primarily upon chromium, copper, gold, rhodium, ruthenium, silver, tantalum, and/or tungsten.
Bias seed layers <b>30</b> and <b>40</b> are each preferably formed of an about 50 Å to about 200 Å thick layer of a material selected to promote the texture and grain growth of each subsequently formed layer. More preferably, bias seed layers <b>30</b> and <b>40</b> are formed of a material such as chromium, ruthenium, tantalum, titanium, tungsten, or an alloy based primarily on chromium, ruthenium, tantalum, titanium, and/or tungsten. Alternatively, bias seed layers <b>30</b> and <b>40</b> may be formed of more than one layer, such as a multi-layer of tantalum and titanium-tungsten or a multi-layer of tantalum and chromium.
Bias layers <b>32</b> and <b>42</b> are each preferably formed of an about 100 Å to about 1000 Å thick layer of a hard magnetic material, such as cobalt-chromium-platinum, cobalt-platinum, or an alloy based primarily upon cobalt-chromium-platinum and/or cobalt-platinum.
Second contacts <b>34</b> and <b>44</b> are each preferably formed of an about 50 Å to about 2000 Å thick layer of a low resistivity material, such as chromium, copper, gold, rhodium, ruthenium, silver, tantalum, tungsten, or an alloy based primarily upon chromium, copper, gold, rhodium, ruthenium, silver, tantalum, and/or tungsten. In a first alternate embodiment of the present invention, first and second dual path conductor/magnet structures <b>20</b> and <b>22</b> do not include second contacts <b>34</b> and <b>44</b>.
Depending upon the material selected for second contacts <b>34</b> and <b>44</b>, a second contact seed layer having similar properties to first contact seed layers <b>26</b> and <b>36</b> may be used to grow second contacts <b>34</b> and <b>44</b>. Accordingly, <figref idref="DRAWINGS">FIG. 2</figref> is a cross-sectional view of transducing head <b>50</b> in accord with a second alternate embodiment of the present invention. Transducing head <b>50</b> is identical to transducing head <b>10</b>, except that it includes first dual path conductor/magnet structure <b>50</b> having second contact seed layer <b>56</b> positioned between bias layer <b>32</b> and second contact <b>34</b> in place of first dual path conductor/magnet structure <b>20</b> and second dual path conductor/magnet structure <b>54</b> having second contact seed layer <b>58</b> positioned between bias layer <b>42</b> and second contact <b>44</b> in place of second dual path conductor/magnet structure <b>22</b>. Elements common to <figref idref="DRAWINGS">FIGS. 1 and 2</figref> are identically numbered.
In a third alternate embodiment of the present invention, first contact seed layer <b>26</b>, first contact <b>28</b>, and bias seed layer <b>30</b> of first dual path conductor/magnet structure <b>20</b> of transducing head <b>10</b> are replaced with a single layer of chromium or ruthenium. Similarly, first contact seed layer <b>36</b>, first contact <b>38</b>, and bias seed layer <b>40</b> of second dual path conductor/magnet structure <b>22</b> of transducing head <b>10</b> are replaced with a single layer of chromium or ruthenium.
Although the present invention can be used with any type of MR sensor requiring longitudinal biasing, it is particularly useful for spin valve sensors. In particular, the transducing head configuration of the present invention allows for lower resistivity pedestals for bias layers <b>32</b> and <b>42</b>, the benefit of which will be described below. In a preferred embodiment, MR sensor <b>16</b> is a spin valve sensor. <figref idref="DRAWINGS">FIGS. 3 and 4</figref> show examples of two different spin valve sensors which may be used with the present invention.
<figref idref="DRAWINGS">FIG. 3</figref> is a layer diagram of spin valve sensor <b>60</b> configured as a bottom spin valve. GMR sensor <b>60</b> is a multi-layered device having pinning layer <b>62</b>, pinned layer <b>64</b>, spacer layer <b>66</b>, and free layer <b>68</b>. Pinning layer <b>62</b> is formed adjacent to pinned layer <b>64</b> to fix a magnetization of pinned layer <b>64</b>. Spacer layer <b>66</b> is positioned between pinned layer <b>64</b> and free layer <b>68</b> to decouple the magnetizations thereof. Pinned layer <b>64</b> is positioned between pinning layer <b>62</b> and spacer layer <b>66</b>.
Pinning layer <b>62</b> is preferably formed of an antiferromagnetic material. Pinned layer <b>64</b> and free layer <b>68</b> are each preferably formed of ferromagnetic materials, and spacer layer <b>66</b> is preferably a thin layer of a nonmagnetic material. Each of the layers of spin valve <b>60</b>, in turn, can be formed of multiple layers as is well known in the art of magnetoresistive sensor design.
The magnetization of pinned layer <b>64</b> is fixed in a predetermined direction while the magnetization of free layer <b>68</b> rotates freely in response to an external magnetic field emanating from a magnetic medium. The magnetization of pinned layer <b>64</b> is pinned by exchange coupling pinning layer <b>62</b> with pinned layer <b>64</b>. A resistance of spin valve <b>60</b> varies as a function of an angle that is formed between the magnetization of free layer <b>68</b> and the magnetization of pinned layer <b>64</b>.
<figref idref="DRAWINGS">FIG. 4</figref> is a layer diagram of a spin valve sensor <b>70</b> configured as a dual spin valve. Spin valve sensor <b>70</b> is a multi-layered device having first pinning layer <b>72</b>, first pinned layer <b>74</b>, first spacer layer <b>76</b>, free layer <b>78</b>, second spacer layer <b>80</b>, second pinned layer <b>82</b>, and second pinning layer <b>84</b>. First pinning layer <b>72</b> is formed adjacent to first pinned layer <b>74</b> to fix a magnetization thereof. Second pinning layer <b>84</b> is similarly formed adjacent to second pinned layer <b>82</b>. Free layer <b>78</b> is positioned between first and second pinned layers <b>74</b> and <b>82</b> such that first spacer layer <b>76</b> separates first pinned layer <b>77</b> from free layer <b>78</b> and second spacer layer <b>80</b> separates free layer <b>78</b> from second pinned layer <b>82</b>. First and second spacer layers <b>76</b> and <b>80</b> serve to decouple free layer <b>78</b> from first and second pinned layers <b>74</b> and <b>82</b>.
First and second pinning layers <b>72</b> and <b>84</b> are each preferably formed of antiferromagnetic materials. First and second pinned layers <b>74</b> and <b>82</b> and free layer <b>78</b> are each preferably formed of ferromagnetic materials. First and second spacer layers <b>76</b> and <b>80</b> are each preferably thin layers of nonmagnetic materials. Each of the layers of spin valve <b>70</b> can be in turn formed of multiple layers.
The magnetization of each of first and second pinned layers <b>74</b> and <b>82</b> are fixed in predetermined directions, preferably parallel to each other, while the magnetization of free layer <b>78</b> rotates freely in response to an external magnetic field emanating from a magnetic medium. The magnetization of first pinned layer <b>74</b> is pinned by exchange coupling first pinning layer <b>72</b> with first pinned layer <b>74</b>. The magnetization of second pinned layer <b>82</b> is pinned by exchange coupling second pinning layer <b>84</b> with second pinned layer <b>82</b>. A resistance of spin valve sensor <b>70</b> varies as a function of the angles that are formed between the magnetization of free layer <b>78</b> and the magnetizations of first and second pinned layers <b>74</b> and <b>82</b>.
To appreciate the advantages presented by the present invention over the prior art, one must first understand the problems associated with prior art designs. <figref idref="DRAWINGS">FIG. 5</figref> is a cross-sectional view of prior art transducing head <b>90</b>. Transducing head <b>90</b> includes first gap layer <b>92</b>, sensor seed layer <b>94</b>, MR sensor <b>96</b>, cap layer <b>98</b>, first conductor/magnet structure <b>100</b>, second conductor/magnet structure <b>102</b>, and second gap layer <b>104</b>.
Sensor seed layer <b>94</b> is formed on a central region of insulating first gap layer <b>92</b>. MR sensor <b>96</b> is formed on sensor seed layer <b>94</b>. Cap layer <b>98</b> is positioned on MR sensor <b>96</b>.
First and second conductor/magnet structures <b>100</b> and <b>102</b> are arranged on end portions of gap layer <b>92</b> in an abutted-junction configuration on opposite sides of MR sensor <b>96</b>. First and second conductor/magnet structures <b>100</b> and <b>102</b> function to provide current to MR sensor <b>96</b> and to provide longitudinal biasing to a sensing layer of MR sensor <b>96</b>. Insulating second gap layer <b>104</b> is positioned over cap layer <b>98</b> and first and second conductor/magnet structures <b>100</b> and <b>102</b>.
First conductor/magnet structure <b>100</b> is sequentially formed of bias seed layer <b>106</b>, bias layer <b>108</b>, and contact <b>110</b>. Similarly, second conductor/magnet structure <b>102</b> is sequentially formed of bias seed layer <b>112</b>, bias layer <b>114</b>, and contact <b>116</b>.
For transducing head <b>90</b> to operate correctly, the sensing layer of MR sensor <b>96</b> must be stabilized against the formation of edge domains since domain wall motion results in electrical noise that makes data recovery impossible. In transducing head <b>90</b>, this stabilization is achieved with a permanent magnet abutted configuration in which bias layers <b>108</b> and <b>114</b> abut opposite sides of MR sensor <b>96</b> to provide longitudinal biasing to the sensing layer of MR sensor <b>96</b>. This function requires that bias layers <b>108</b> and <b>114</b> have sufficient magnetic flux to provide a magnetic field adequate to magnetically stabilize and maintain in a single domain state the sensing layer of MR sensor <b>96</b>. Specifically, bias layers <b>108</b> and <b>114</b> must have sufficiently high remnant magnetization (M<sub>r</sub>) to stabilize the sensing layer of MR sensor <b>96</b> and sufficiently high resistance to demagnetization (H<sub>c</sub>) to remain magnetized during its normal course of operation. Critical to meeting these requirements are the properties of bias seed layers <b>106</b> and <b>112</b>. For this reason, when fabricating transducing head <b>90</b>, bias layers <b>108</b> and <b>114</b> are deposited prior to contacts <b>110</b> and <b>116</b>. This sequence allows for better control of the properties of bias seed layers <b>106</b> and <b>112</b>. This arrangement of bias layers <b>108</b> and <b>114</b> beneath contacts <b>110</b> and <b>116</b> also allows for better longitudinal alignment of the sensing layer of MR sensor <b>96</b> with bias layers <b>108</b> and <b>114</b>.
Difficulties have arisen with this prior art design, however, as a reader width of MR sensor <b>96</b> has decreased to accommodate ever increasing areal densities of magnetic media. Namely, this design has contributed to an increase in overall resistivity of transducing head <b>90</b> as the reader width has decreased. During fabrication of transducing head <b>90</b>, prior to deposition of first and second conductor/magnet structures <b>100</b> and <b>102</b>, a pattern of photoresist is deposited over cap layer <b>98</b> to define the reader width of MR sensor <b>96</b>. This decrease in this width has required the reduction in a thickness of first and second conductor/magnet structures <b>100</b> and <b>102</b>, and in particular, a thickness of contacts <b>110</b> and <b>116</b> to enable the removal of the photoresist pattern. This decrease in thickness of contacts <b>110</b> and <b>116</b> has resulted in an increase in overall resistivity of transducing head <b>90</b>.
Thus, the present invention is a novel configuration of a transducing head's bias and conductor layers that allows for a reduction in overall resistivity of the transducing head while still sufficiently biasing an MR sensor of the transducing head. The present invention alters the structure of prior art transducing head <b>90</b> by improving upon first and second conductor/magnet structures <b>100</b> and <b>102</b>. Specifically, first and second dual path conductor/magnet structures <b>20</b> and <b>22</b> of the present invention differ from that of prior art first and second conductor/magnet structures <b>100</b> and <b>102</b> in that the structure of present invention has bias layer <b>32</b> interspersed between first contact <b>28</b> and second contact <b>34</b> and bias layer <b>42</b> interspersed between first contact <b>38</b> and second contact <b>44</b>. This configuration of the present invention thus allows for a path of low resistivity current flow adjacent MR sensor <b>16</b> and for a decrease in overall MR sensor resistivity, while still providing for sufficient stabilization of MR sensor <b>16</b>.
A key element of the present invention is the recognition that bias layers <b>32</b> and <b>42</b> can be formed subsequent to first contacts <b>28</b> and <b>38</b> through the selection of a suitable materials for first contact seed layers <b>26</b> and <b>36</b> and bias seed layers <b>30</b> and <b>40</b>. Bias layers <b>32</b> and <b>42</b> each preferably have a high resistance to thermal degradation, a coercivity (H<sub>c</sub>) between about 1 kOe and about 5 kOe, and an in-plane remnant squareness (S), which is a ratio of remnant magnetization (M<sub>r</sub>) to saturation magnetization (M<sub>s</sub>), greater than about 0.8. To achieve these properties, first contact seed layers <b>26</b> and <b>36</b> and bias seed layers <b>30</b> and <b>40</b> preferably promote in respective bias layers <b>32</b> and <b>42</b> a crystallographic growth with the [0001] direction in the plane of bias layers <b>32</b> and <b>42</b>. Without such careful selection of the materials for bias seed layers <b>30</b> and <b>40</b>, it would be impossible to form bias layers <b>32</b> and <b>42</b> with the preferred properties. For instance, bias layers <b>32</b> and <b>42</b> will not properly perform if deposited over first contacts <b>28</b> and <b>38</b> formed of gold without careful selection of a suitable material for bias seed layers <b>30</b> and <b>40</b>.
An additional advantage of the present invention is that overall resistivity of transducing head <b>10</b> is not as greatly affected during fabrication as that of prior art transducing head <b>90</b>. A transducing head is typically formed by (a) depositing a plurality of layers that will form a MR sensor, (b) patterning a reader width of the MR sensor, (c) depositing a conductor/magnet structure on opposite sides of the MR sensor, and (d) defining a back edge of the MR sensor. During step (d), portions of the top-most layers in certain regions of the overall transducing head are often removed, causing an increase in overall resistivity of the transducing head.
This reduction in thickness is illustrated in <figref idref="DRAWINGS">FIGS. 6 and 7</figref>. <figref idref="DRAWINGS">FIG. 6</figref> is a cross-sectional view of transducing head <b>10</b> of <figref idref="DRAWINGS">FIG. 1</figref> taken along cross-section VI—VI, and <figref idref="DRAWINGS">FIG. 7</figref> is a cross-sectional view of prior art transducing head <b>90</b> of <figref idref="DRAWINGS">FIG. 5</figref> taken along cross-section VII—VII. With prior art transducing head <b>90</b>, the top-most layer of second conductor/magnet structure <b>102</b> is low-resistivity contact <b>116</b>, which when thinned along portion <b>126</b>, leaves only significantly higher resistivity bias layer <b>114</b> along portion <b>126</b>. Conversely, with transducing head <b>10</b> of the present invention, the top-most layers are contact <b>44</b> and bias layer <b>42</b>. During step (d), second contact <b>44</b> will be completely removed along portion <b>122</b>, bias layer <b>42</b> will be thinned along portion <b>122</b>, and low resistivity first contact <b>38</b> will not be thinned.
<figref idref="DRAWINGS">FIGS. 8 and 9</figref> are charts comparing resistivity of transducing head <b>10</b> to the resistivity of prior art transducing head <b>90</b>. As illustrated in <figref idref="DRAWINGS">FIG. 8</figref>, prior to application of step (d) described above, the resistivity of portion <b>120</b> (adjacent the air bearing surface) of transducing head <b>10</b> is about 80% that of portion <b>124</b> of prior art transducing head <b>90</b>. More significantly, as illustrated in <figref idref="DRAWINGS">FIG. 9</figref>, after application of milling step (d), the resistivity of portion <b>122</b> (distant the air bearing surface) of transducing head <b>10</b> is about 20% that of portion <b>126</b> of prior art transducing head <b>90</b>. The examples of <figref idref="DRAWINGS">FIGS. 8 and 9</figref> are merely representative of a single embodiment of transducing heads <b>10</b> and <b>90</b>. However, <figref idref="DRAWINGS">FIGS. 8 and 9</figref> do illustrate that the dual-path conductor/magnet structure of the present invention has a significant impact on the resistivity of the transducing head in the region that has been milled to define the back edge of the transducing head.
Another advantage of the present invention is an increase in MR sensor signal strength. A pedestal of a transducing head is defined as those layers of the transducing head that elevate a bias layer of the transducing head. By using lower resistivity pedestals, an increase in current through the MR sensor can be achieved, thus increasing the MR sensor signal amplitude. In prior art transducing head <b>90</b>, the pedestal for bias layer <b>42</b> is formed exclusively of bias seed layer <b>106</b>. In contrast, in transducing head <b>10</b> of the present invention, the pedestal for bias layer <b>42</b> includes first contact seed layer <b>36</b>, first contact <b>38</b> and bias seed layer <b>40</b>. As the pedestal of transducing head <b>10</b> is formed primarily of relatively low resistivity first contact <b>38</b>, it will have a substantially lower resistivity than the pedestal of prior art transducing head <b>90</b>.
<figref idref="DRAWINGS">FIG. 10</figref> is a graph illustrating current distribution through a spacer layer of spin valve sensor of a transducing head. Displayed on the horizontal axis is the first 30 Å, measured from an edge toward a center, of a 100 ÅA wide spin valve sensor. Displayed on the vertical axis is current density along the width of the spin valve sensor. Curve <b>130</b> illustrates current density in a spin valve sensor having relatively high resistivity pedestals, while curve <b>132</b> illustrates current density in a spin valve sensor having relatively low resistivity pedestals. As shown in <figref idref="DRAWINGS">FIG. 10</figref>, a greater amount of current flows through the spin valve sensor corresponding to the lower resistance pedestals of the present invention. Thus, the transducing head configuration of the present invention allows for greater read sensitivity.
Although the present invention has been described with reference to preferred embodiments, workers skilled in the art will recognize that changes may be made in form and detail without departing from the spirit and scope of the invention.
Contents5
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| US8964336B2 | Cited by | United States of America | Search report |
| US2004047082A1 | Cited by | United States of America | Pre-grant |
| US9190080B1 | Cited by | United States of America | Applicant |
| US2008137237A1 | Cited by | United States of America | Pre-grant |
| US8385025B2 | Cited by | United States of America | Applicant |
| US5508866A | Cites | United States of America | Applicant |
| US5528440A | Cites | United States of America | Applicant |
| US5742459A | Cites | United States of America | Applicant |
| US5784225A | Cites | United States of America | Applicant |
| US5883764A | Cites | United States of America | Applicant |
| US5936810A | Cites | United States of America | Search report |
| US6055138A | Cites | United States of America | Applicant |
| US6094325A | Cites | United States of America | Applicant |
| US6219207B1 | Cites | United States of America | Search report |
| US6229678B1 | Cites | United States of America | Applicant |
| WO9916057A1 | Cites | World Intellectual Property Organization (WIPO) | Applicant |
| U.S. Appl. No. 10/012,829, filed Dec. 10, 2001, Seigler et al. | Non-patent | – | Third party observation |
| U.S. Appl. No. 10/012,829, filed Dec. 10, 2001, Seigler et al. | Non-patent | – | Applicant |
2 members in 1 office
Priority claims6
| Document | Office | Kind | Date |
|---|---|---|---|
| 29754201 | United States of America | P | |
| 29754201 | United States of America | P | |
| 14256302 | United States of America | A | |
| 60297542 | – | – | – |
| US20010297542P | – | – | – |
| US20020142563 | – | – | – |
Members2
| Document | Office | Kind | |
|---|---|---|---|
| US2002186516A1 | United States of America | A1 | |
| US6954343B2This record | United States of America | B2 |
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Numbers
- Publication
- 06954343
- Publication, DOCDB
- 6954343
- Publication, EPODOC
- US6954343
- Application
- 10142563
- Application, DOCDB
- 14256302
- Application, EPODOC
- US20020142563
Titles
- English
- Magnetoresistive sensor having low resistivity dual path conductor and optimized magnetic
Patent term adjustment
- A delay
- +414 daysthe office missed an examination deadline
- Net adjustment
- 414 days
Classification
- CPC, 3
- G11B5/3903
- G11B5/313
- G11B5/3932
- IPC, 2
- G11B5 31
- G11B5 39
- USPC, 3
- 360324120
- G9B005114
- G9B005115